Devices and methods for speckle reduction in scanning projectors

ABSTRACT

Devices and methods are described herein that use a first solid figure element, a polarizing beam splitter, and a second solid figure element or array of mirrors to reduce speckle in projected images. Specifically, laser light is generated and split into two portions having orthogonal polarizations. The first portion of laser light is reflected in the second solid figure element or the array of mirrors and is then spatially recombined with the second portion of laser light in the first solid figure element. The difference in path length followed by the two portions generates a temporal incoherence in the recombined laser light beam, and that temporal incoherence reduces speckle in the projected image.

PRIORITY CLAIM

This application is a continuation-in-part of and claims priority to U.S. patent application Ser. No. 15/096,791, filed Apr. 12, 2016, which is hereby incorporated by reference in its entirety.

FIELD

The present disclosure generally relates to projectors, and more particularly relates to scanning laser projectors.

BACKGROUND

In scanning laser projectors, pixels are typically generated by modulating light from laser light sources as a scanning mirror scans the modulated light in a raster pattern. One continuing issue in scanning laser projectors is “speckle”. In general, speckle is an image artifact that can reduce the quality of projected images. Speckle occurs when a coherent light source is projected onto a randomly diffusing surface. When highly coherent light reflects off a rough surface, various components of the light combine to form patches of higher intensity light and lower intensity light. To the human eye or other detector with a finite aperture, these patches of variable intensity appear as speckles, as some small portions of the image look brighter than other small portions. Furthermore, these intensity differences can vary depending on observer's position, and thus the speckles can appear to change when the observer moves.

As such, speckle can significantly reduce the quality of image generated by a coherent source, such as laser in a scanning laser projector.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a schematic diagram of a scanning laser projector in accordance with various embodiments of the present invention;

FIGS. 2A and 2B show schematic views of a speckle reduction component in accordance with various embodiments of the present invention;

FIGS. 3A, 3B, 3C and 3D show schematic views of speckle reduction components in accordance with various embodiments of the present invention;

FIGS. 4A, 4B, 4C, 4D, 4E, and 4F show schematic views of speckle reduction components in accordance with various embodiments of the present invention;

FIGS. 5A and 5B shows a schematic view of a scanning laser projector in accordance with various embodiments of the present invention;

FIG. 6 shows a plan view of a microelectromechanical system (MEMS) device with a scanning mirror in accordance with various embodiments of the present invention;

FIG. 7 shows a block diagram of a mobile device in accordance with various embodiments of the present invention;

FIG. 8 shows a perspective view of a mobile device in accordance with various embodiments of the present invention;

FIG. 9 shows a perspective view of a head-up display system in accordance with various embodiments of the present invention;

FIG. 10 shows a perspective view of eyewear in accordance with various embodiments of the present invention;

FIG. 11 shows a perspective view of a gaming apparatus in accordance with various embodiments of the present invention; and

FIG. 12 shows a perspective view of a gaming apparatus in accordance with various embodiments of the present invention.

DESCRIPTION OF EMBODIMENTS

In general, the embodiments described herein provide a scanning laser projector that reduces speckle to improve image quality. In general, the scanning laser projector generates a temporal incoherence in the laser light beam used to project an image, and that temporal incoherence reduces speckle in the projected image.

In one embodiment, a speckle reduction component is included in the scanning laser projector, where the speckle reduction component includes a polarizing beam splitter positioned between a first solid figure element and a second solid figure element. In another embodiment, a speckle reduction component includes a polarizing beam splitter positioned between a first solid figure element and an array of mirrors. In yet another embodiment, a speckle reduction component includes a polarizing beam splitter positioned between a first solid figure element and both a second solid figure element and an array of mirrors.

In general, the speckle reduction component is configured to split the laser light into a first portion of the laser light having P polarization and a second portion of the laser light having S polarization. The first portion of laser light is reflected off at least three faces then spatially recombined with the second portion of laser light in the first solid figure element. The recombined light beams are then passed to at least one scanning mirror and reflected into a raster pattern of scan lines to form a projected image.

In one embodiment, the splitting of the laser light into a first portion and a second portion, where the first portion is internally reflected off three internal faces of the second solid figure element before being spatially recombined with the first portion, generates a relative delay between the two portions. When the two portions are recombined, this relative delay results in a temporal incoherence between the two portions in the recombined laser light beam. This temporal incoherence reduces speckle in the projected image. Specifically, the temporal incoherence of the two recombined light beams, where the two recombined light beams have an orthogonal polarization orientation, effectively creates two uncorrelated speckle patterns in the projected image. These two uncorrelated speckle patterns partially average out and thus reduce the amount of speckle that is apparent to a viewer of the projected image. Furthermore, the various embodiments can provide such a speckle reduction in a relatively compact sized device and with relatively high optical power efficiency. Specifically, the embodiments provide the delay with internal reflection on at least three faces of the second solid figure element. As will be described in greater detail below, the internal reflection off at least three faces of the second solid figure element can provide the temporal delay needed to effectively reduce speckle in the projected image while having relatively small dimensions. Furthermore, the internal reflection off at least three faces facilitates low optical power loss, and thus can provide the temporal delay needed to effectively reduce speckle in the projected image while maintaining relatively high efficiency.

In another embodiments, the splitting of the laser light into a first portion and a second portion, where the first portion is internally reflected off the at least two surfaces of the array of mirrors before being spatially recombined with the first portion, generates a relative delay between the two portions. When the two portions are recombined, this relative delay results in a temporal incoherence between the two portions in the recombined laser light beam. This temporal incoherence again reduces speckle in the projected image. Specifically, the temporal incoherence of the two recombined light beams, where the two recombined light beams have an orthogonal polarization orientation, effectively creates two uncorrelated speckle patterns in the projected image. These two uncorrelated speckle patterns partially average out and thus reduce the amount of speckle that is apparent to a viewer of the projected image.

As with the previous embodiment, this embodiment can provide such a speckle reduction in a relatively compact sized device and with relatively high optical power efficiency. Furthermore, this embodiment can facilitate improved alignment of the two recombined light beams. Specifically, by precisely positioning the at least two surfaces in the array of mirrors the first portion and the second portion of the laser light can be made to be precisely coaxial when recombined in the first solid figure element. Facilitating the first portion and the second portion of the laser light into a precisely coaxial recombined beam can improve the resulting image quality in the scanning laser projector. For example, this can improve image quality by keeping the combined beam size as small as possible (e.g., as close as possible to the original size of each component beam).

Specifically, in a scanning laser projector the beam size determines the minimum pixel size, and thus determine the maximum resolution. Thus, providing a relatively small beam small can reduce pixel size and improve resolution. Thus, when the two recombined beams are coaxial and overlapping then the recombined beam is as small as possible and the resolution improved. In contrast, if the recombined beams are not coaxial they would appear larger and could worsen the resulting resolution.

Turning now to FIG. 1, a schematic diagram of a scanning laser projector 100 is illustrated. The scanning laser projector 100 includes a laser light source 102, scanning mirror(s) 104, a drive circuit 106, and a speckle reduction component 108. During operation, the laser light source 102 provides a beam of laser light is encoded with pixel data to generate image pixels that are to be projected by the scanning laser projector 100. To facilitate this, the drive circuit 106 controls the movement of the scanning mirror(s) 104. Specifically, the drive circuit 106 provides excitation signal(s) to excite motion of the scanning mirror(s) 104.

The scanning mirror(s) 104 reflect the laser light beam into an image region 112. Specifically, during operation of the scanning light projector 100, the scanning mirror(s) 104 are controlled by the drive circuit 106 to reflect the beams of laser light into a raster pattern 114. This raster pattern 114 of laser light beam generates a projected image. In general, the horizontal motion of the beam of laser light in this raster pattern 114 define rows of pixels in the projected image, while the vertical motion of the beams of laser light in the raster pattern 114 defines a vertical scan rate and thus the number of rows in the projected image.

In accordance with the embodiments described herein, the speckle reduction component 108 is inserted into the optical path of the scanning laser projector 100 to reduce speckle in the projected image. In one embodiment, the speckle reduction component includes a polarizing beam splitter positioned between a first solid figure element and a second solid figure element. In another embodiment, a speckle reduction component includes a polarizing beam splitter positioned between a first solid figure element and/or an array of mirrors. The first solid figure element is configured to receive the laser light beam and pass that the laser light beam to the polarizing beam splitter. The polarizing beam splitter passes a first portion of the laser light beam having P polarization to the second solid figure element and/or array of mirrors, and reflects a second portion of the laser light beam having S polarization back to the first solid figure element. The first portion of the laser light beam received by the second solid figure element and/or array of mirrors is reflected off at least three surfaces, and then outputted back to first solid figure element, where the first portion of light is spatially recombined with the second portion of laser light in the first solid figure element. The scanning mirror(s) 104 are configured to reflect the recombined laser light beam, and the drive circuit 106 is configured to provide an excitation signal to excite motion of the scanning mirror(s) 104. Specifically, the motion is excited such that the scanning mirror(s) 104 reflect the recombined laser light beam in the raster pattern 114 of scan lines to form a projected image

In such embodiments, the splitting of the laser light into a first portion and a second portion, where the first portion is internally reflected off three internal faces of the second solid figure element or off at least two surfaces of the array of mirrors before being spatially recombined with the first portion, generates a relative delay between the two portions. Specifically, the first portion of the laser light beam is temporally delayed relative to the second portion that reflects off the polarizing beam splitter. This relative delay between the portions of the laser light beam generates a temporal incoherence when the light beams are recombined. That temporal incoherence continues when the recombined light beams are scanned by scanning mirror(s) 104 into the raster pattern 114 to project an image.

This temporal incoherence in the recombined laser beams that are scanned to project an image results in reduced speckle in the projected image. Specifically, the temporal incoherence of the two recombined light beams, where the two recombined light beams have an orthogonal polarization orientation, effectively creates two uncorrelated speckle patterns in the projected image. These two uncorrelated speckle patterns partially average out and thus reduce the amount of speckle that is apparent to a viewer of the projected image.

Turning now to FIG. 2A, a more detailed embodiment of a speckle reduction component 200 is illustrated. The speckle reduction component 200 includes a polarization adjuster 202, a first solid figure element 204, a second solid figure element 206, and a polarizing beam splitter 208. Again, the speckle reduction component 200 is inserted into the optical path of a scanning laser projector to reduce speckle in the projected image. Specifically, the speckle reduction component 200 is configured to receive laser light from a laser light source 102 and output laser light to the scanning mirrors 104. When so configured, the speckle reduction component 200 will reduce speckle in the projected image.

It should be noted that while FIG. 2A shows the speckle reduction component receiving the laser light directly from the laser light source 102, that this is just one example embodiment. In other embodiments there can be additional optical elements inserted between the laser light source 102 and the speckle reduction component 200. Furthermore, there can be additional optical elements inserted between the speckle reduction component 200 and the scanning mirrors 104. Specific examples of such other elements will be discussed in greater detail below with reference to the detailed embodiments illustrated in FIGS. 4 and 5.

In general, the speckle reduction component 200 uses the polarization adjuster 202, the first solid figure element 204, the second solid figure element 206, and the polarizing beam splitter 208 to introduce a temporal incoherence in the laser light used to project the image, with that temporal incoherence implemented to reduce speckle in the projected image.

Specifically, in this embodiment the laser light source 102 provides a laser light beam, and the polarization adjuster 202 is configured to adjust the polarization of the laser light beam such that it includes power along two orthogonal polarization directions. As such, a variety of different types of devices and components can be used to implement the polarization adjuster 202. For example, both polarization converters and polarization rotators can be used to implement the polarization adjuster 202. Examples of polarization converters that can be used include quarter-wave plates and depolarizers. Examples of polarization rotators that can be used include half-wave plates and configurations that rotate the laser light source 102. In each case, such a polarization adjuster 202 can be implemented to provide the laser light beam with orthogonal polarization components. Furthermore, as will be described in greater detail below, it is generally desirable to implement the polarization adjuster 202 such that the resulting laser light beam has nearly equal optical power in two orthogonal polarization directions. For example, such that the laser light beam has S and P polarization components with half of the overall optical power in each component.

As noted above, in one example a quarter-wave plate can be used to implement the polarization adjuster 202. Specifically, a quarter-wave plate can be implemented to convert linear polarized light from the light source 102 to circularly polarized light, where circularly polarized light has orthogonal polarization components with substantially equal optical power. In general, a quarter-wave plate is fabricated to include different indices of refraction for different orientations of light. When linearly polarized light passes through a quarter-wave plate these different indices of refraction cause some polarizations to propagate slower than others. Specifically, to implement a quarter-wave plate, the indices of refraction and dimensions of the quarter-wave plate are selected to introduce a phase shift of 90 degrees (π/2 radians) between orthogonal polarizations. Such a configuration will cause linearly polarized light to be converted to circular polarized light and vice versa, and thus can be used as the polarization adjuster 202.

In another implementation, the polarization adjuster 202 can be implemented with a half-wave plate that is configured to rotate polarization by 45 degrees (π/4 radians) relative to the polarization direction of the polarizing beam splitter 208. Such an implementation is equivalent to the rotating the laser light source 102 relative to the polarization direction of polarizing beam splitter 208, and thus can be used to provide for the splitting of the laser light beam into components with nearly equal optical power based on the two orthogonal polarization directions.

In yet another implementation, the polarization adjuster 202 can be implemented with a polarizing element that divides the laser light beam power between two orthogonal polarizations. For example, a depolarizer such as a depolarizing filter or polarization scrambling device can be configured to scramble the polarization such that it includes two orthogonal polarization directions can be implemented as the polarization adjuster 202.

The first solid figure element 204 is configured to receive the laser light beam and pass that the laser light beam to the polarizing beam splitter 208. The polarizing beam splitter 208 splits the incoming laser light beam based on polarization, passing a first portion of the laser light beam having P polarization to the second solid figure element 206, and reflects a second portion of the laser light beam having S polarization back to the first solid figure element 204. The first portion of the laser light beam received by the second solid figure element 206 is internally reflected off at least three internal faces of the second solid figure element 206. After being internally reflected off at least three faces, the first portion of the laser light is outputted back to first solid figure element 204. At the first solid figure element 204, the first portion of light is spatially recombined with the second portion of laser light.

It should be noted that the polarizing beam splitter 208 preferably splits the incoming laser light beam into two portions with equal optical power. Stated another way, the polarizing beam splitter 208 allows approximately half the power to travel into the second solid figure element 206 while the other half of the power is immediately reflected back into the first solid figure element 204. This equal optical power splitting can improve the effectiveness of the speckle reduction by facilitating that the two generated speckle patterns will have approximately equal brightness and thus can more effectively average out and reduce the overall speckle of the projected image. Such an equal power split can be provided by having substantially equal power orthogonal polarization components in the laser light that is applied to the polarizing beam splitter 208. For example, using laser light having a circular polarization with substantially equal magnitude P and S polarization components will result in an equal optical power split at the polarizing beam splitter 208.

As noted above, the second solid figure element 206 is configured such that the first portion of laser light is reflected off at least three internal faces before exiting and recombining in with the second portion of laser light in the second solid figure element 206. As one example, this can be implemented with a second solid figure element 206 that comprises four faces. In such an implementation a first face of the four faces can be positioned adjacent to first solid figure element 204, while a second face, a third face and a fourth face of the four faces are configured to internally reflect the first portion of the laser light.

In such an embodiment, the second solid figure element 206 can comprise a polyhedron, such as a cubic polyhedron. In a cubic polyhedron embodiment, the four faces would each be of equal length, with equal angles between faces, and the first portion of light would reflect off three faces before reentering the first solid figure element 204 at the fourth face. Of course, this is just one example, and in other embodiments the second solid figure element 206 can be configured with more than four faces. For example, the second solid figure element 206 can be implemented with five or more faces. As more specific examples, the second solid figure element 206 can be implemented with 8 faces or 12 faces. In an 8 faced embodiment, the first portion of the laser light would internally reflect off 7 faces before reentering the first solid figure element 204 at the 8^(th) face. In such an embodiment, the 8 faces would have 135 degree angles between faces. In a 12 faced embodiment, the first portion of the laser light would internally reflect off 11 faces before reentering the first solid figure element 204 at the 12^(th) face. In such an embodiment, the 12 faces would have 150 degree angles between faces.

In all of these various embodiments, the relatively high number of internal reflections occurring in the second solid figure element 206 can facilitate a relatively large temporal delay to the first portion of the laser light relative to second portion of the laser light. Furthermore, this relatively large temporal delay can be provided in a relatively small device size. Specifically, providing reflection off at least three faces of the second solid figure element 206 can facilitate the needed temporal delay to effectively reduce speckle in the projected image while having relatively small dimensions. Thus, the embodiments described herein can provide effective speckle reduction in a compact and size effective speckle reduction component.

Furthermore, in all of these various embodiments, the relatively high number of internal reflections occurring in the second solid figure element 206 can facilitate relatively high optical power efficiency. It is generally desirable to implement the second solid figure element 206 in a way that reduces optical power loss, and thus improves overall optical power efficiency in the speckle reduction component 200. One way to reduce optical power loss is to increase the percentage of the first light portion that reflects around the second solid figure element 206 and is recombined with the first light portion in the first solid figure element 204. The embodiments described herein can reduce optical power loss and improve efficiency by using total internal reflection (TIR) to internally reflect the first light portion inside the second solid figure element 206. When TIR occurs, almost all the optical power is reflected, with only relatively small optical power losses occurring due to factors such as surface and material imperfections. Thus, using TIR in the second solid figure element 206 can reduce loss, and thus can improve optical power efficiency of the speckle reduction component 200.

In general, TIR occurs when the light is coming from more optically dense material (with a relatively high index of refraction n), is incident upon less optically dense material (with a relatively low index of refraction n), and the angle of incidence is sufficiently large. Specifically, to facilitate TIR in the second solid figure element 206, the angle of incidence at each internally reflected face must be greater than a critical angle θ_(C) (measured from a normal to the reflecting face) where the critical angle θ_(C) is defined as:

$\theta_{C} = {\arcsin\left( \frac{n_{2}}{n_{1}} \right)}$ where n₁ is the refractive index of the second solid figure element 206, and n₂ is the refractive index of the material outside the second solid figure element 206. As one specific example, the second solid figure element 206 is made of glass with a refractive index of n₁=1.52, the air outside the second solid figure element 206 has a refractive index of n₂=1.00, and thus the critical angle θ_(C) is approximately 41 degrees. Thus, in such an embodiment the angle of incidence at each reflecting face in the second solid figure element 206 must be greater than approximately 41 degrees to ensure TIR.

The embodiments described herein facilitate the use of TIR to provide relatively high optical power efficiency. Specifically, by including at least four faces in the second solid figure element 206, and reflecting the first portion of light off at least three faces, relatively high angles of incidence inside the second solid figure element 206 are provided. As one example, a second solid figure element 206 with four equal length faces can have angles of incidences of 45 degrees, significantly greater than the minimum required for a glass/air interface to have TIR. Likewise, a second solid figure element 206 with eight equal length faces can have angles of incidences of 67.5 degrees, again significantly greater than the minimum required for a glass/air interface to have TIR. Examples of such implementations will be discussed below with reference to FIGS. 3A-3D.

Furthermore, to facilitate TIR and reduce losses due to surface imperfections, it is generally desirable for each reflecting face to be polished or otherwise be processed to increase the smoothness of the reflecting face. In such embodiments any suitable technique for polishing the reflecting surface may be used.

It should be noted that while TIR is just one technique that can be used to provide internal reflection in the second solid figure element 206 that other techniques can be used. For example, ordinary reflection at each reflecting face can instead be facilitated with reflective coatings that can be applied using any suitable technique. However, such other techniques are likely to result in greater optical power loss compared to the use of TIR.

The first solid figure element 204 can likewise be implemented in a variety of shapes. In general, the first solid figure element 204 provides an input path to the polarizing beam splitter 208, and then provides for the recombining of the first and second portions of the laser beam. As one example shape that can be implemented to provide this, the first solid figure element 204 can be implemented in the shape of a prism. In such an embodiment, the first solid figure element 204 would have an input face and an output face, where the input face receives the laser light beam and the output face outputs the recombined laser light beam. In such an embodiment a third face of the first solid figure element 204 can provide the interface to the second solid figure element 206. As will be discussed in greater detail below, the polarizing beam splitter 208 can be implemented by applying one or more coatings to such a third face.

In general, the polarizing beam splitter 208 is implemented to split the incoming laser light into two portions, with the first portion passing to the second solid figure element 206, and the second portion reflecting back into the first solid figure element 204. Preferably, the polarizing beam splitter 208 is implemented in a way that provides an equal optical power split between light that is passed to the second solid figure element 206 and light that is reflected back into the first solid figure element 204. This can be accomplished by converting the incoming light to have S and P polarization components, and then implementing the polarizing beam splitter 208 to pass P polarized components and reflect S polarized components. Such a polarizing beam splitter 208 can be implemented by applying one or more coatings the first solid figure element 204 and/or the second solid figure element 206. For example, various dielectric coatings can be applied to the face(s) of these element(s) to implement the polarizing beam splitter 208, and then optical cement can be used to bond those elements together.

The first solid figure element 204 and the second solid figure element 206 are each implemented with materials that are transparent to the wavelengths provided by the laser light source 102. For example, the first solid figure element 204 and the second solid figure element 206 can be made from isotropic glass or isotropic plastic. Finally, various antireflective coatings can be applied to the input and output surfaces of the first solid figure element 204.

The splitting of the laser light into a first portion and a second portion by the polarizing beam splitter 208, where the first portion is internally reflected off three internal faces of the second solid figure element 206 before being spatially recombined with the first portion in the first solid figure element 204, generates a relative delay between the two portions. Specifically, the first portion of the laser light beam that reflects off at least three internal surfaces is temporally delayed relative to the second portion that reflects off the polarizing beam splitter. This relative delay between light beams generates a temporal incoherence when the light beams are recombined. That temporal incoherence continues when the recombined light beams are passed to the scanning mirrors 104 for scanning into the raster pattern to project an image.

This temporal incoherence in the recombined laser beams that are scanned to project an image results in reduced speckle in the projected image. Specifically, the temporal incoherence of two recombined light beams, where the light beams have orthogonal polarization components, effectively creates two speckle patterns, one for each of the two separated light beams. Because each of those two speckle patterns is essentially random and uncorrelated, when recombined the two speckle patterns will partially average out, reducing the amount of speckle that is apparent to a viewer of the projected image.

Specifically, in a typical embodiment such an implementation can reduce the apparent speckle by a factor of √2. This level of speckle reduction can be achieved when the first solid figure element 204 provides an approximately 50/50 optical power split and the relative delay between the two beams is at least equal or greater to the coherence length of the laser light. In general, the coherence length is the propagation distance over which a coherent wave maintains coherence. In one embodiment, with a light source having a Lorentz function distribution (as is common with laser diodes), such a coherence length L_(C) is defined as:

$L_{c} = \frac{\lambda^{2}}{\pi\;\Delta\;\lambda}$ where λ is the central wavelength of the laser light, and Δλ is the full width half maximum (FWHM) spectral bandwidth of the laser light. Thus, in a typical embodiment, the first solid figure element 204 and the second solid figure element 206 are sized and otherwise configured to provide a relative delay that is at least equal to the coherence length L_(C). For example, for a visible laser diode light source with a few nanometers of FWHM spectrum bandwidth, the coherence length would typically be on the order of a few 100 μm. Thus, a few millimeters of path difference provided in the second solid figure element 206 should generally be sufficient to break the coherence length of such a light source.

As was noted above, the various embodiments described herein can provide such a temporal delay in a relatively compact structure and with relatively high power efficiency. Specifically, the relatively high number of internal reflections occurring in the second solid figure element 206 can facilitate a temporal delay that is both large relative to the size of the device and with relatively low optical power losses. Thus, the embodiments described herein can provide effective speckle reduction in a compact and size effective speckle reduction component with high power efficiency.

Turning now to FIG. 2B, a more detailed embodiment of a second embodiment speckle reduction component 250 is illustrated. This embodiment is similar to that of FIG. 2A but uses an array of mirrors to provide reflection. Two or more surfaces in the array of mirrors can be precisely positioned to make the resulting recombined beam more coaxial.

The speckle reduction component 250 includes a polarization adjuster 202, a first solid figure element 204, an array of mirrors 260, and a polarizing beam splitter 208. Again, the speckle reduction component 250 is inserted into the optical path of a scanning laser projector to reduce speckle in the projected image. Specifically, the speckle reduction component 250 is configured to receive laser light from a laser light source 102 and output laser light to the scanning mirrors 104. When so configured, the speckle reduction component 250 will reduce speckle in the projected image.

In general, the speckle reduction component 250 uses the polarization adjuster 202, the first solid figure element 204, the array of mirrors 260, and the polarizing beam splitter 208 to introduce a temporal incoherence in the laser light used to project the image, with that temporal incoherence implemented to reduce speckle in the projected image. In general, the polarization adjuster 202, the first solid figure element 204, and the polarizing beam splitter 208 each operate as described and can include the various features described above with reference to FIG. 2.

Again, the first solid figure element 204 is configured to receive the laser light beam and pass that the laser light beam to the polarizing beam splitter 208. The polarizing beam splitter 208 splits the incoming laser light beam based on polarization, passing a first portion of the laser light beam having P polarization to the array of mirrors 260, and reflects a second portion of the laser light beam having S polarization back to the first solid figure element 204. The first portion of the laser light beam received by the array of mirrors 260 is reflected off at least two precisely positioned surfaces. After being reflected off at least two precisely positioned surfaces, the first portion of the laser light is outputted back to first solid figure element 204. At the first solid figure element 204, the first portion of light is spatially recombined with the second portion of laser light.

It should again be noted that the polarizing beam splitter 208 preferably splits the incoming laser light beam into two portions with equal optical power. Stated another way, the polarizing beam splitter 208 allows approximately half the power to travel into the array of mirrors 260 while the other half of the power is immediately reflected back into the first solid figure element 204. This equal optical power splitting can again improve the effectiveness of the speckle reduction by facilitating that the two generated speckle patterns will have approximately equal brightness and thus can more effectively average out and reduce the overall speckle of the projected image.

As was noted above, this embodiment uses mirrors 260 to facilitate precise recombining of the first portion of light with the second portion of light into a coaxial combined laser beam. These mirrors can be implemented with any suitable material, including coated glass and coated plastics. In some embodiments these mirrors can be affixed using adhesives that provide for precise positioning of the mirrors. For example, the mirrors can be affixed into the precise needed position while the adhesive cures. In one specific example that will be described below, the mirrors can be affixed to solid optical elements with index matching adhesives. In other examples, the mirrors can be affixed to a substrate.

The array of mirrors 260 is configured such that the first portion of laser light is reflected off at least two precisely positioned surfaces before exiting and recombining in with the second portion of laser light in the first solid figure element 204. As one example, the array of mirrors 260 can be implemented with at least two mirrors, where the at least two of the mirrors are each precisely positioned to make the recombined beams coaxial. It should be noted that the precise positioning of two mirrors is sufficient because the laser beam propagates in a straight line, and such a line can be defined with a position and an angle. Specifically, by precisely positioning two mirrors the first mirror can be positioned to define where the beam hits the second mirror, and the second mirror can be used to define the angle at which the beam leaves the second mirror. Thus, the precise positioning of two mirrors is typically sufficient to define the straight line of the beam and make the recombined beams coaxial.

It should be noted that while the precise positioning of at least two of the mirrors is typically sufficient to make the recombined beams coaxial, the array of mirrors can include additional mirrors. Again, such mirrors can be mounted independently or they can be attached to the surfaces of a second solid figure element. Examples of such embodiments will be discussed below with reference to FIGS. 4A, 4B, 4C, and 4D.

A variety of different techniques can be used to facilitate the precise positioning of the at least two mirrors. In general, the first solid figure element 204, the polarizing beam splitter 208 can be positioned on a subassembly. The at least two mirrors can then be aligned and then glued with a suitable adhesive. For example, an index matching adhesive that cures when exposed UV light can be used. In such an embodiment the at least two mirrors can be precisely positioned relative to the first solid figure element 204 and the polarizing beam splitter 208 then exposed to UV light while holding the mirrors in position.

In other examples additional reflections can be provided by the second solid figure element having one or more surfaces that are configured for total internal reflection. Examples of such embodiments will be discussed with reference to FIGS. 4E and 4F. Again, in such an embodiment the two mirrors can be precisely positioned to make the recombined beams coaxial.

Turning now to FIG. 3A, a top view of a specific implementation of a speckle reduction component 300 is illustrated. In this illustrated implementation, the speckle reduction component 300 includes a polarization adjuster 302, a first solid figure element 304, a second solid figure element 306, and a polarizing beam splitter 308. The speckle reduction component 300 is an example of the type of device that can be inserted into the optical path of a scanning laser projector to reduce speckle in the projected image. In such an application the speckle reduction component 300 is configured to receive laser light from a laser light source and output laser light to one or more scanning mirrors. When so implemented, the speckle reduction component 300 will reduce speckle in the projected image and thus provide for improved image quality.

In general, the speckle reduction component 300 uses the polarization adjuster 302, the first solid figure element 304, the second solid figure element 306, and the polarizing beam splitter 308 to introduce a temporal incoherence in the laser light used to project the image, with that temporal incoherence implemented to reduce speckle in the projected image.

Specifically, in this illustrated embodiment a laser light source (not shown in FIG. 3A) provides a laser light beam, and the polarization adjuster 302 is configured to convert the laser light beam to have equal optical power orthogonal polarization components. As one specific example, the polarization adjuster 302 comprises a quarter-wave plate configured to convert linearly polarized light to circularly polarized light, where circular polarized light has substantially equal S and P polarization components that are out of phase.

In the specific embodiment of FIG. 3A, the first solid figure element 304 comprises a prism element, the second solid figure element 306 comprises a polyhedron element, and the polarizing beam splitter 308 comprises a coating applied between the first solid figure element 304 and the second solid figure element 306. Thus, during operation, the polarized light beam impacts the first solid figure element 304 at an input surface 310. In this illustrated embodiment, the polarized light beam is perpendicular to the input surface 310, and thus passes into the first solid figure element 304 without significant reflection. The polarized light beam propagates through the first solid figure element 304 until it impacts the polarizing beam splitter 308. At the polarizing beam splitter 308, the light of one polarization component (i.e., the P polarization component) passes through to the second solid figure element 306, while the light of the other polarization component (i.e., the S polarization component) is reflected back into the first solid figure element 304.

Inside the second solid figure element 306, the P polarization component continues and passes through the second solid figure element 306 until it impacts the face 312. At the face 312, the P polarization component internally reflects to the face 314, where it reflects again to face 316, where it reflects for a final time and continues back to the polarizing beam splitter 308. In this embodiment, the path taken by the P polarization component as it reflects off the faces 312, 314 and 316 introduces a delay to the P polarization component of the laser light.

This temporally delayed portion of the laser light exits the second solid figure element 306 and again crosses the polarizing beam splitter 308 and reenters the first solid figure element 304. After reentering the first solid figure element 304, the P polarization component of the laser light spatially recombines with the S polarization component of the laser light that was reflected by the polarizing beam splitter 308. This recombined laser light beam passes through the first solid figure element 304 until it exits at the output face 318. It should be noted that this in this embodiment, the recombined laser light beam exits at a perpendicular angle to the output face 318.

Notably, the P polarization component travels along a path that is significantly longer than the S polarization component before exiting the first solid figure element 204. This longer path length is facilitated by the shape of the second solid figure element 306 and the internal reflection that occurs inside the second solid figure element 306. Because of this longer path, the P polarization light beam will be delayed in time relative to the S polarization light beam when recombined at the output surface. This generates a temporal incoherence in the recombined light beam, and that temporal incoherence continues when the recombined light beam is scanned to project an image. Furthermore, because the P polarization light beam and the S polarization light beam have orthogonal polarization orientation, that temporal incoherence in the recombined light beam will result in two uncorrelated speckle patterns in the projected image. These two uncorrelated speckle patterns will partially average out and thus reduce the amount of speckle that is apparent to a viewer of the projected image.

Furthermore, the embodiment illustrated in FIG. 3A can provide such a speckle reduction in a relatively compact device. Specifically, by reflecting three times off the internal faces of the second solid figure element 306, a relatively large temporal delay is provided in a second solid figure element 306 that is relatively compact. Furthermore, by reflecting three times off the internal faces the second solid figure element 306 facilitates internal angles of incidences of 45 degrees, significantly greater than the minimum required for a typical glass/air interface to have total internal reflection (TIR). Thus, this embodiment can provide effective speckle reduction in a compact and size effective speckle reduction component, and with relatively low optical power losses.

Turning now to FIG. 3B, a top view of another specific implementation of a speckle reduction component 320 is illustrated. This embodiment is similar to that illustrated in FIG. 3A, but can also be implemented to provide spatial shaping of the laser light beam.

It should be first noted that many commonly used laser light sources produce beams with non-circular spatial distributions. For example, many laser diodes produce laser light beams with elliptical (but non-circular) spatial distribution, and such a spatial distribution is not ideal for many scanning laser projectors. For these reasons, it can be desirable to provide a mechanism for spatially shaping the laser light beam in a way that makes the laser light beam more circularized.

In this illustrated implementation, the speckle reduction component 320 includes a polarization adjuster 322, a first solid figure element 324, a second solid figure element 326, and a polarizing beam splitter 308. Again, the speckle reduction component 330 is an example of the type of device that can be inserted into the optical path of a scanning laser projector to reduce speckle in the projected image.

The major difference in the embodiment of FIG. 3B is the shape of the first solid figure element 324. Specifically, in this illustrated embodiment, the first solid figure element 324 has unbalanced dimensions implemented to shape the recombined laser light beam. Specifically, the shape of the first solid FIG. 324 is such that the recombined output laser light beam exits the output surface 332 at a non-orthogonal angle. Exiting the output surface 332 at a non-orthogonal angle causes refraction, which compresses the existing spatial distribution of the laser light beam. This compression of the spatial distribution of the laser light beam can be used to provide beam circularization. Specifically, the compression can be used to circularize a laser light beam that otherwise would have a non-circular elliptical spatial distribution, and can thus shape of the laser light beam for more effective use in the scanning laser projector. Thus, the speckle reduction component 320 can provide both speckle reduction and beam circularization in one relatively compact device.

Turning now to FIG. 3C, a top view of another specific implementation of a speckle reduction component 350 is illustrated. In this illustrated implementation, the speckle reduction component 350 includes a polarization adjuster 352, a first solid figure element 354, a second solid figure element 356, and a polarizing beam splitter 358. Again, the speckle reduction component 350 is an example of the type of device that can be inserted into the optical path of a scanning laser projector to reduce speckle in the projected image.

As with the embodiments of FIGS. 3A and 3B, the embodiment shown in FIG. 3C users internal reflection of the laser light beam in the second solid figure element 356 to introduce a delay in that portion of the laser light beam. When such a delay is large enough, the delay will cause a temporal incoherence in the laser light used to project the image, with that temporal incoherence provided to reduce speckle in the projected image.

In FIG. 3C, the shape of the first solid figure element 354 and the second solid figure element 356 are different than those illustrated in FIG. 3A. Specifically, instead of a pure prism and a pure cubic shape respectively, these elements have “cut off corners” at various locations. These cut off corners show how exterior shape of the solid figure elements can be changed while still providing speckle reduction. Specifically, in FIG. 3C the number of faces determines the internal reflection and resulting path length for the first portion of the laser light. Thus, the temporal incoherence is provided even if the first solid figure element 354 is not a pure prism or if the second solid figure element 356 is not a pure cubic. Instead, the number and configurations of faces used to reflect the first portion of light and the resulting amount of introduced delay determines the temporal incoherence that is provided by speckle reduction component.

Again, the introduced delay generates a temporal incoherence in the recombined light beam, and that temporal incoherence continues when the recombined light beam is scanned to project an image. The resulting final temporal incoherence of light beams having an orthogonal polarization orientation effectively creates two speckle patterns in the projected image, and because each of those two speckle patterns are uncorrelated, the two speckle patterns will partially average out, reducing the amount of speckle that is apparent to a viewer of the projected image.

Turning now to FIG. 3D, a top view of another specific implementation of a speckle reduction component 370 is illustrated. In this illustrated implementation, the speckle reduction component 370 includes a polarization adjuster 372, a first solid figure element 374, a second solid figure element 376, and a polarizing beam splitter 378.

In general, the speckle reduction component 370 uses the polarization adjuster 372, the first solid figure element 374, the second solid figure element 376, and the polarizing beam splitter 378 to introduce a temporal incoherence in the laser light used to project the image, with that temporal incoherence implemented to reduce speckle in the projected image.

In the specific embodiment of FIG. 3D, the second solid figure element 376 has 8 faces, and the first portion of light (having P polarization) internally reflects off 7 of those eight faces before reentering the first solid figure element 374 and being recombined with the second portion of light (having S polarization). By reflecting off 7 faces, the relative path difference is increased and thus, compared to the embodiments of FIG. 3A, the speckle reduction component 370 can provide an even greater relative temporal delay. Furthermore, increasing the number of faces increases the angle of incidence at each face, and such an increase in the angle of incidence can increase the percentage of light reflected at each face, and thus can facilitate the providing of total internal reflection inside the second solid figure element 376.

Again, such a temporal delay generates a temporal incoherence in the recombined light beam, and that temporal incoherence continues when the recombined light beam is scanned to project an image. This temporal incoherence effectively creates two speckle patterns in the projected image, reducing the amount of speckle that is apparent to a viewer of the projected image. Furthermore, the embodiment illustrated in FIG. 3D can provide such a speckle reduction in a relatively compact device and high power efficiency. Specifically, by reflecting seven times off the internal faces of the second solid figure element 376, a relatively large temporal delay is provided in a second solid figure element 376. Additionally, by reflecting seven times off the internal faces of the second solid figure element 376, relatively large angles of incidences of 67.5 degrees are provided, thus facilitating total internal reflection (TIR) and low optical power losses.

Turning now to FIG. 4A, a top view of another specific implementation of a speckle reduction component 400 is illustrated. In this illustrated implementation, the speckle reduction component 400 includes a polarization adjuster 402, a first solid figure element 404, an array of mirrors 406, and a polarizing beam splitter 408. The speckle reduction component 400 is again an example of the type of device that can be inserted into the optical path of a scanning laser projector to reduce speckle in the projected image.

In general, the speckle reduction component 400 uses the polarization adjuster 402, the first solid figure element 404, the array of mirrors 406, and the polarizing beam splitter 408 to introduce a temporal incoherence in the laser light used to project the image, with that temporal incoherence implemented to reduce speckle in the projected image.

Specifically, in this illustrated embodiment a laser light source (not shown in FIG. 4A) provides a laser light beam, and the polarization adjuster 402 is configured to convert the laser light beam to have equal optical power orthogonal polarization components. As one specific example, the polarization adjuster 402 comprises a quarter-wave plate configured to convert linearly polarized light to circularly polarized light, where circular polarized light has substantially equal S and P polarization components that are out of phase.

In the specific embodiment of FIG. 4A, the first solid figure element 404 comprises a prism element, the array of mirrors 406 comprises an array of three mirrors 407, and the polarizing beam splitter 408 comprises a coating applied to the first solid figure element 404 and the second solid figure element 406. Thus, during operation, the polarized light beam impacts the first solid figure element 404 at an input surface 410. In this illustrated embodiment, the polarized light beam is perpendicular to the input surface 410, and thus passes into the first solid figure element 404 without significant reflection. The polarized light beam propagates through the first solid figure element 404 until it impacts the polarizing beam splitter 408. At the polarizing beam splitter 408, the light of one polarization component (i.e., the P polarization component) passes through to the array of mirrors 406, while the light of the other polarization component (i.e., the S polarization component) is reflected back into the first solid figure element 404.

In the array of mirrors 406, the P polarization component continues until it impacts the reflecting surface 412. At the reflecting surface 412, the P polarization component reflects to the reflecting surface 414, where it reflects again to reflecting surface 416, where it reflects for a final time and continues back to the polarizing beam splitter 408. In this embodiment, the path taken by the P polarization component as it reflects off the reflecting surfaces 412, 414 and 416 introduces a delay to the P polarization component of the laser light.

This temporally delayed portion of the laser light exits the array of mirrors 406 and again crosses the polarizing beam splitter 408 and reenters the first solid figure element 404. After reentering the first solid figure element 404, the P polarization component of the laser light spatially recombines with the S polarization component of the laser light that was reflected by the polarizing beam splitter 408. This recombined laser light beam passes through the first solid figure element 404 until it exits at the output surface 418. It should be noted that this in this embodiment, the recombined laser light beam exits at a perpendicular angle to the output surface 418.

Notably, the P polarization component travels along a path that is significantly longer than the S polarization component before exiting the first solid figure element 404. This longer path length is facilitated by the arrangement of the array of mirrors 406 and the reflection that occurs at each of the surfaces 412, 414 and 416. Because of this longer path, the P polarization light beam will be delayed in time relative to the S polarization light beam when recombined at the output surface. This generates a temporal incoherence in the recombined light beam, and that temporal incoherence continues when the recombined light beam is scanned to project an image. Furthermore, because the P polarization light beam and the S polarization light beam have orthogonal polarization orientation, that temporal incoherence in the recombined light beam will result in two uncorrelated speckle patterns in the projected image. These two uncorrelated speckle patterns will partially average out and thus reduce the amount of speckle that is apparent to a viewer of the projected image.

Furthermore, in this embodiment, the array of mirrors 406 can be precisely configured to make the recombined beams coaxial. In this illustrated example, each of array of mirrors 406 is can be positioned independently. By precisely controlling the position of at least two mirrors (and thus two of the surfaces 412, 414 and 416) in the array of mirrors 406 the P polarization light beam and the S polarization light beam can be made coaxial when recombined in the first solid figure element 404. Again, this functionally recreates a single beam, and such beam can provide good image quality compared to beams that are not coaxial.

Turning now to FIG. 4B, a top view of another specific implementation of a speckle reduction component 415 is illustrated. This embodiment is similar to that illustrated in FIG. 4A, but also includes a second solid figure element 409, and each of the mirrors 407 are attached to a surface of the second solid figure element 409.

In this particular example, the second solid figure element 409 comprises a cubic polyhedron element, and the polarizing beam splitter 408 comprises a coating applied between the first solid figure element 404 and the second solid figure element 409. Thus, during operation, the polarized light beam impacts the first solid figure element 404 at an input surface 410. In this illustrated embodiment, the polarized light beam is again perpendicular to the input surface 410, and thus passes into the first solid figure element 404 without significant reflection. The polarized light beam propagates through the first solid figure element 404 until it impacts the polarizing beam splitter 408. At the polarizing beam splitter 408, the light of one polarization component (i.e., the P polarization component) passes through to the second solid figure element 409, while the light of the other polarization component (i.e., the S polarization component) is reflected back into the first solid figure element 404.

Inside the second solid figure element 409, the P polarization component continues and passes through the second solid figure element 406 until it impacts the reflecting surface 412 of the mirror 407. At the reflecting surface 412, the P polarization component reflects to the reflecting surface 414 of the next mirror 407, where it reflects again to reflecting surface 416 of the last mirror 407, where it reflects for a final time and continues back to the polarizing beam splitter 408. In this embodiment, the path taken by the P polarization component as it reflects off the reflecting surfaces 412, 414 and 416 introduces a delay to the P polarization component of the laser light.

This temporally delayed portion of the laser light exits the second solid figure element 409 and again crosses the polarizing beam splitter 408 and reenters the first solid figure element 404. After reentering the first solid figure element 404, the P polarization component of the laser light spatially recombines with the S polarization component of the laser light that was reflected by the polarizing beam splitter 408. This recombined laser light beam passes through the first solid figure element 404 until it exits at the output surface 418.

The P polarization component travels along a path that is significantly longer than the S polarization component before exiting the first solid figure element 404. This again generates a temporal incoherence in the recombined light beam, and that temporal incoherence continues when the recombined light beam is scanned to project an image. Furthermore, because the P polarization light beam and the S polarization light beam have orthogonal polarization orientation, that temporal incoherence in the recombined light beam will result in two uncorrelated speckle patterns in the projected image. These two uncorrelated speckle patterns will partially average out and thus reduce the amount of speckle that is apparent to a viewer of the projected image.

Like the embodiment of FIG. 4A, this embodiment allows the array of mirrors 406 to be precisely positioned to make the recombined beams coaxial. Again, in this illustrated example, each of array of mirrors 406 is mounted to a corresponding surface of the second solid body element 409 and can be positioned independently relative to the corresponding surfaces.

A variety of different techniques can be used to facilitate the precise and independent positioning of at least two mirrors 407 in the array of mirrors 406. For example, each of the mirrors 407 can be attached to the second solid figure element 409 with index matching adhesive. Such an index matching adhesive allows the light beam to pass through the surface of the second solid figure element 409 and impact the surface of the mirror. Thus, the reflection is actually caused by the surface of the mirror and not by internal reflection in the second solid figure element 409.

As one specific example, the index matching adhesive can be one that cures when exposed to UV or other light. In such an embodiment the first solid figure element 404, polarizing beam splitter 408, and second solid figure element 409 can first be bonded together. Then, each of the mirrors 407 can be precisely positioned relative to the corresponding surface of the second solid figure element 409. The assembly can then be exposed to UV light while holding the mirrors in position. When the adhesive is cured the mirrors 407 are permanently attached the precise positions relative to the surfaces of the second solid figure element 409. Thus, the completed assembly is made with at least two of the mirrors 407 precisely positioned relative to their corresponding faces in a way that will make the recombined beams substantially coaxial.

It should also be noted that this technique can allow the mirrors to be positioned with greater accuracy than would be found in the surfaces of the second solid figure element 409. For example, each of the surfaces on the second solid figure element 409 may be accurate to +/−0.01 degree, while the mirrors 407 can be positioned to achieve a potential accuracy of +/−0.001. This again can be used to make the recombined beams more coaxial then could be achieved using only the surfaces of the second solid figure element 409.

Furthermore, the use of such an adhesive allows each mirror 407 to be attached at a slight angle relative to the corresponding surface of the second solid figure element 409. For example, each mirror 407 can be precisely positioned by holding it the desired angle relative to the surface of the second solid figure element 409 until the adhesive sets. When the adhesive sets the mirror 407 is permanently attached the precise angle needed to make the recombined beams substantially coaxial.

It should again be noted in this configuration the precise arrangement of at least two of the mirrors 407 will generally be sufficient to make the recombined beams coaxial. Thus, one of the mirrors 407 can be attached directly against the second solid figure element 409, and the other two mirrors 407 positioned at desired angles relative to the surfaces while the adhesive sets. Thus, by precisely controlling the position of at least two of the mirrors 407 (and their corresponding surfaces 412, 414 and 416) in the array of mirrors 406 the P polarization light beam and the S polarization light beam can be made coaxial when recombined in the first solid figure element 404.

Turning now to FIG. 4C, a top view of another specific implementation of a speckle reduction component 417 is illustrated. This embodiment is similar to that illustrated in FIG. 4A, but also includes a second solid figure element 411 in the shape of a prism. Also, in this embodiment the polarizing beam splitter 408 comprises a coating applied between the first solid figure element 404 and the second solid figure element 411. Compared to the embodiment of FIG. 4A, placing the polarizing beam splitter 408 between solid figure elements 404 and 411 facilitates wideband beam splitting without causing different colors to refract at different angles. Thus, such an embodiment can be made to work with a combined laser beam that includes multiple colors (e.g., RGB).

This embodiment otherwise operates in the same manner as that illustrated in FIG. 4A. Furthermore, in this embodiment the array of mirrors 406 can again be precisely positioned to make the recombined beams coaxial. In this illustrated example, each of array of mirrors 406 can again be positioned independently. By precisely controlling the position of at least two mirrors 406 and the corresponding surfaces the P polarization light beam and the S polarization light beam are made coaxial when recombined in the first solid figure element 404.

Turning now to FIG. 4D, a top view of another specific implementation of a speckle reduction component 420 is illustrated. This embodiment is similar to that illustrated in FIG. 4A, but can also be implemented to provide spatial shaping of the laser light beam.

It again should be first noted that many commonly used laser light sources produce beams with non-circular spatial distributions. In this illustrated embodiment, the first solid figure element 424 has unbalanced dimensions implemented to shape the recombined laser light beam. Specifically, the shape of the first solid FIG. 424 is such that the recombined output laser light beam exits the output surface 442 at a non-orthogonal angle. Exiting the output surface 442 at a non-orthogonal angle causes refraction, which compresses the existing spatial distribution of the laser light beam. This compression of the spatial distribution of the laser light beam can be used to provide beam circularization. Specifically, the compression can be used to circularize a laser light beam that otherwise would have a non-circular elliptical spatial distribution, and can thus shape of the laser light beam for more effective use in the scanning laser projector. Thus, the speckle reduction component 420 can provide both speckle reduction and beam circularization in one relatively compact device.

Turning now to FIG. 4E, a top view of another specific implementation of a speckle reduction component 450 is illustrated. In this illustrated implementation, the speckle reduction component 450 includes a polarization adjuster 452, a first solid figure element 454, a second solid figure element 456, an array of mirrors 457, and a polarizing beam splitter 458. Again, the speckle reduction component 450 is an example of the type of device that can be inserted into the optical path of a scanning laser projector to reduce speckle in the projected image.

This embodiment differs from the embodiments in FIGS. 4A and 4B in that it uses internal reflection of the laser light beam in the second solid figure element 456. Specifically, the mirrors 457 provide for two reflections, while the total internal reflection on the surface of the second solid figure element 456 provides a third reflection. Thus, in this embodiment only two mirrors are required.

Again, in this embodiment the mirrors 457 can again be precisely positioned to make the recombined beams coaxial. Specifically, by precisely controlling the position the two mirrors 457 the P polarization light beam and the S polarization light beam are made coaxial when recombined in the first solid figure element 454.

Also, In FIG. 4E, the shape of the first solid figure element 454 and the second solid figure element 456 are different than those illustrated in FIG. 4A. Specifically, instead of a pure prism and a pure cubic shape respectively, these elements have “cut off corners” at various locations. These cut off corners show how exterior shape of the solid figure elements can be changed while still providing speckle reduction.

Turning now to FIG. 4F, a top view of another specific implementation of a speckle reduction component 470 is illustrated. In this illustrated implementation, the speckle reduction component 470 includes a polarization adjuster 472, a first solid figure element 474, a second solid figure element 476, mirrors 477, and a polarizing beam splitter 478.

In this embodiment, the mirrors 477 provide for two reflections, while the total internal reflection on the surface of the second solid figure element 476 provides five reflections. Again, in this embodiment the mirrors 477 can be precisely positioned to make the recombined beams coaxial. By precisely controlling the position the two mirrors 477 the P polarization light beam and the S polarization light beam are made coaxial when recombined in the first solid figure element 454.

Specifically, in the specific embodiment of FIG. 4F, the second solid figure element 476 has 8 surfaces, and the first portion of light (having P polarization) internally reflects off five of those eight surfaces. Two of the other surfaces have mirrors 477 attached. Thus, the P polarization light internally reflects of five surfaces of the second solid figure element 476 and two mirrors 477 before reentering the first solid figure element 474 and being recombined with the second portion of light (having S polarization). By reflecting off 5 internal surfaces and two mirrors, the relative path difference is increased and thus, compared to the embodiments of FIG. 4A, the speckle reduction component 470 can provide an even greater relative temporal delay. Furthermore, increasing the number of surfaces increases the angle of incidence at each surface, and such an increase in the angle of incidence can increase the percentage of light reflected at each surface, and thus can facilitate the providing of total internal reflection inside the second solid figure element 476.

Again, such a temporal delay generates a temporal incoherence in the recombined light beam, and that temporal incoherence continues when the recombined light beam is scanned to project an image. This temporal incoherence effectively creates two speckle patterns in the projected image, reducing the amount of speckle that is apparent to a viewer of the projected image. Furthermore, the embodiment illustrated in FIG. 4F can provide such a speckle reduction in a relatively compact device and high power efficiency. Specifically, by reflecting five times off the internal surfaces of the second solid figure element 476 and two mirrors 477 coupled to the other surfaces, a relatively large temporal delay is provided in a second solid figure element 476.

Turning now to FIG. 5A, a schematic view of a scanning laser projector 700 is illustrated. The scanning laser projector 700 is a more detailed example of the type of system that can be used in accordance with various embodiments of the present invention. Scanning laser projector 700 includes an image processing component 702, a pixel drive generator 704, a red laser module 706, a green laser module 708, and a blue laser module 710. Light from the three laser modules is combined with dichroics 712, 714, and 716. Scanning laser projector 700 also includes fold mirror 718, drive circuit 720, and MEMS device 722 with scanning mirror 724.

In operation, image processing component 702 processes video content at using two dimensional interpolation algorithms to determine the appropriate spatial image content for each scan position at which an output pixel is to be displayed by the pixel drive generator. For example, the video content may represent a grid of pixels at any resolution (e.g., 640×480, 848×480, 1280×720, 1920×1080). The input light intensity encoding typically represents the light intensity in 8, 10, 12 bit or higher resolutions.

This content is then mapped to a commanded current for each of the red, green, and blue laser sources such that the output intensity from the lasers is consistent with the input image content. In some embodiments, this process occurs at output pixel rates in excess of 150 MHz. The laser beams are then directed onto an ultra-high speed gimbal mounted 2 dimensional bi-axial laser scanning mirror 724. In some embodiments, this bi-axial scanning mirror is fabricated from silicon using MEMS processes. The vertical axis of rotation is operated quasi-statically and creates a vertical sawtooth raster trajectory. The vertical axis is also referred to as the slow-scan axis. The horizontal axis is operated on a resonant vibrational mode of the scanning mirror. In some embodiments, the MEMS device uses electromagnetic actuation, achieved using a miniature assembly containing the MEMS die and small subassemblies of permanent magnets and an electrical interface, although the various embodiments are not limited in this respect. For example, some embodiments employ electrostatic or piezoelectric actuation. Any type of mirror actuation may be employed without departing from the scope of the present invention.

The horizontal resonant axis is also referred to as the fast-scan axis. In some embodiments, raster pattern 726 is formed by combining a sinusoidal component on the horizontal axis and a sawtooth component on the vertical axis. In these embodiments, output beam 728 sweeps back and forth left-to-right in a sinusoidal pattern, and sweeps vertically (top-to-bottom) in a sawtooth pattern with the display blanked during flyback (bottom-to-top).

It should be noted that FIG. 7 illustrates the sinusoidal pattern as the beam sweeps vertically top-to-bottom, but does not show the flyback from bottom-to-top. In other embodiments, the vertical sweep is controlled with a triangular wave such that there is no flyback. In still further embodiments, the vertical sweep is sinusoidal. The various embodiments of the invention are not limited by the waveforms used to control the vertical and horizontal sweep or the resulting raster pattern 726.

The drive circuit 720 provides a drive signal to MEMS device 722. The drive signal includes an excitation signal to control the resonant angular motion of scanning mirror 724 on the fast-scan axis, and also includes slow scan drive signal to cause deflection on the slow-scan axis. The resulting mirror deflection on both the fast and slow-scan axes causes output beam 728 to generate a raster scan 726 in an image region 730. In operation, the laser light sources produce light pulses for each output pixel and scanning mirror 724 reflects the light pulses as beam 728 traverses the raster pattern 726. Drive circuit 720 also receives a feedback signal from MEMS device 722. The feedback signal from the MEMS device 722 can describe the maximum deflection angle of the mirror, also referred to herein as the amplitude of the feedback signal. This feedback signal is provided to the drive circuit 720, and is used by the drive circuit 720 to accurately control the motion of the scanning mirror 724.

In operation, drive circuit 720 excites resonant motion of scanning mirror 724 such that the amplitude of the feedback signal is constant. This provides for a constant maximum angular deflection on the fast-scan axis as shown in raster pattern 726. The excitation signal used to excite resonant motion of scanning mirror 724 can include both amplitude and a phase. Drive circuit 720 includes feedback circuit(s) that modifies the excitation signal amplitude to keep the feedback signal amplitude substantially constant. Additionally, the drive circuit 720 can modify the excitation signal to control the horizontal phase alignment and vertical position of the raster pattern 726.

To facilitate this, drive circuit 720 may be implemented in hardware, a programmable processor, or in any combination. For example, in some embodiments, drive circuit 720 is implemented in an application specific integrated circuit (ASIC). Further, in some embodiments, some of the faster data path control is performed in an ASIC and overall control is provided by a software programmable microprocessor.

It should be noted that while FIG. 5A illustrates an embodiment with a single MEMS device 722 and a single scanning mirror 724, that this is just one example implementation. As another example, a scanning laser projector could instead be implemented with scanning mirror assembly that includes two scanning mirrors, with one mirror configured to deflect along one axis and another mirror configured to deflect along a second axis that is largely perpendicular to the first axis.

Such an embodiment could include a second MEMS device, a second scanning mirror, and a second drive circuit. The first scanning mirror could be configured to generate horizontal scanning motion, and the second scanning mirror configured to generate vertical motion. Thus, the motion of one scanning mirror determines the horizontal scan amplitude and the motion of the other scanning mirror determines the vertical scan amplitude.

Finally, although red, green, and blue laser light sources are shown in FIG. 7A, the various embodiments are not limited by the wavelength of light emitted by the laser light sources. For example, in some embodiments, non-visible light (e.g., infrared light) is emitted instead of, or in addition to, visible light.

In accordance with the embodiments described herein, a speckle reduction component 740 is inserted into the optical path. The speckle reduction component can be implemented with any of the various embodiments described above. As such, the speckle reduction component 740 uses solid figure elements to reduce speckle in the projected image generated by the scanning laser projector 700. Specifically, the speckle reduction component 740 uses a first solid figure element and a second solid figure element as described with reference to the various embodiments above. The speckle reduction component 740 is configured to receive laser light from the laser modules 706, 708, and 710, and separate the laser light into two components with different relative delays. This relative delay introduces a temporal incoherence in the recombined light beams, and that temporal incoherence results in reduced speckle in the projected image.

It should be noted that in this embodiment the speckle reduction component 740 operates on the laser light after the laser light of different colors (from red laser module 706, a green laser module 708, and a blue laser module 710) have been combined with the dichroics 712, 714, and 716. However, this is just one example, and other embodiments are possible.

For example, turning now to FIG. 5B, a second schematic view of a scanning laser projector 700 is illustrated. The scanning laser projector 750 is another example of the type of system that can be used in accordance with various embodiments of the present invention. Scanning laser projector 750 is similar to that of projector 700 illustrated in FIG. 5A, but instead uses three separate speckle reduction components 752, 754 and 756. Specifically, the scanning laser projector 750 uses separate speckle reduction components 752, 754 and 756, with one for each color laser outputted by the red laser module 706, a green laser module 708, and a blue laser module 710. Again, this is just one example of how such speckle reduction components can be implemented into a scanning laser projector.

Turning now to FIG. 6, a plan view of a microelectromechanical system (MEMS) device with a scanning mirror is illustrated. MEMS device 800 includes fixed platform 802, scanning platform 840, and scanning mirror 816. Scanning platform 840 is coupled to fixed platform 802 by flexures 810 and 812, and scanning mirror 16 is coupled to scanning platform 840 by flexures 820 and 822. Scanning platform 840 has a drive coil connected to drive lines 850, which are driven by a drive signal provided from a drive circuit (e.g., drive circuit 720). The drive signal includes an excitation signal to excite resonant motion of scanning mirror 816 on the fast-scan axis, and also includes a slow-scan drive signal to cause non-resonant motion of scanning platform 840 on the slow-scan axis. Current drive into drive lines 850 produces a current in the drive coil. In operation, an external magnetic field source (not shown) imposes a magnetic field on the drive coil. The magnetic field imposed on the drive coil by the external magnetic field source has a component in the plane of the coil, and is oriented non-orthogonally with respect to the two drive axes. The in-plane current in the coil windings interacts with the in-plane magnetic field to produce out-of-plane Lorentz forces on the conductors. Since the drive current forms a loop on scanning platform 840, the current reverses sign across the scan axes. This means the Lorentz forces also reverse sign across the scan axes, resulting in a torque in the plane of and normal to the magnetic field. This combined torque produces responses in the two scan directions depending on the frequency content of the torque.

The long axis of flexures 810 and 812 form a pivot axis. Flexures 810 and 812 are flexible members that undergo a torsional flexure, thereby allowing scanning platform 840 to rotate on the pivot axis and have an angular displacement relative to fixed platform 802. Flexures 810 and 812 are not limited to torsional embodiments as shown in FIG. 6. For example, in some embodiments, flexures 810 and 812 take on other shapes such as arcs, “S” shapes, or other serpentine shapes. The term “flexure” as used herein refers to any flexible member coupling a scanning platform to another platform (scanning or fixed), and capable of movement that allows the scanning platform to have an angular displacement with respect to the other platform.

Scanning mirror 816 pivots on a first axis formed by flexures 820 and 822, and pivots on a second axis formed by flexures 810 and 812. The first axis is referred to herein as the horizontal axis or fast-scan axis, and the second axis is referred to herein as the vertical axis or slow-scan axis. In some embodiments, scanning mirror 816 scans at a mechanically resonant frequency on the horizontal axis resulting in a sinusoidal horizontal sweep. Further, in some embodiments, scanning mirror 816 scans vertically at a nonresonant frequency, so the vertical scan frequency can be controlled independently.

In a typical embodiment the MEMS device 800 will also incorporates one or more integrated piezoresistive position sensors. For example, piezoresistive sensor 880 can be configured to produces a voltage that represents the displacement of mirror 816 with respect to scanning platform 840, and this voltage can be provided back to the drive circuit. Furthermore, in some embodiments, positions sensors are provided on one scan axis while in other embodiments position sensors are provided for both axes.

It should be noted that the MEMS device 800 is provided as an example, and the various embodiments of the invention are not limited to this specific implementation. For example, any scanning mirror capable of sweeping in two dimensions to reflect a light beam in a raster pattern may be incorporated without departing from the scope of the present invention. Also for example, any combination of scanning mirrors (e.g., two mirrors: one for each axis) may be utilized to reflect a light beam in a raster pattern. Further, any type of mirror drive mechanism may be utilized without departing from the scope of the present invention. For example, although MEMS device 800 uses a drive coil on a moving platform with a static magnetic field, other embodiments may include a magnet on a moving platform with drive coil on a fixed platform. Further, the mirror drive mechanism may include an electrostatic drive mechanism.

The scanning laser projectors described above (e.g., scanning laser projector 100 of FIG. 1) can be implemented in a wide variety of devices and for a wide variety of applications. Several specific examples of these types of devices will not be discussed with reference to FIGS. 7-12. In each case, the various embodiments described above can be implemented with or as part of such a device.

Turning to FIG. 7, a block diagram of a mobile device 900 in accordance with various embodiments is illustrated. Specifically, mobile device 900 is an example of the type of device in which a scanning laser projector as described above can be implemented (e.g., scanning laser projector 100, scanning laser projector 700). As shown in FIG. 7, mobile device 900 includes wireless interface 910, processor 920, memory 930, and scanning laser projector 902. Scanning laser projector 902 includes photodetector(s) configured in an over scanned region signal to provide feedback signal(s) as described above. Scanning laser projector 902 may receive image data from any image source.

For example, in some embodiments, scanning laser projector 902 includes memory that holds still images. In other embodiments, scanning laser projector 902 includes memory that includes video images. In still further embodiments, scanning laser projector 902 displays imagery received from external sources such as connectors, wireless interface 910, a wired interface, or the like.

Wireless interface 910 may include any wireless transmission and/or reception capabilities. For example, in some embodiments, wireless interface 910 includes a network interface card (NIC) capable of communicating over a wireless network. Also for example, in some embodiments, wireless interface 910 may include cellular telephone capabilities. In still further embodiments, wireless interface 910 may include a global positioning system (GPS) receiver. One skilled in the art will understand that wireless interface 910 may include any type of wireless communications capability without departing from the scope of the present invention.

Processor 920 may be any type of processor capable of communicating with the various components in mobile device 900. For example, processor 920 may be an embedded processor available from application specific integrated circuit (ASIC) vendors, or may be a commercially available microprocessor. In some embodiments, processor 920 provides image or video data to scanning laser projector 100. The image or video data may be retrieved from wireless interface 910 or may be derived from data retrieved from wireless interface 910. For example, through processor 920, scanning laser projector 902 may display images or video received directly from wireless interface 910. Also for example, processor 920 may provide overlays to add to images and/or video received from wireless interface 910, or may alter stored imagery based on data received from wireless interface 910 (e.g., modifying a map display in GPS embodiments in which wireless interface 910 provides location coordinates).

Turning to FIG. 8, a perspective view of a mobile device 1000 in accordance with various embodiments is illustrated. Specifically, mobile device 1000 is an example of the type of device in which a scanning laser projector as described above can be implemented (e.g., scanning laser projector 100, scanning laser projector 700). Mobile device 1000 may be a hand held scanning laser projector with or without communications ability. For example, in some embodiments, mobile device 1000 may be a scanning laser projector with little or no other capabilities. Also for example, in some embodiments, mobile device 1000 may be a device usable for communications, including for example, a cellular phone, a smart phone, a tablet computing device, a global positioning system (GPS) receiver, or the like. Further, mobile device 1000 may be connected to a larger network via a wireless (e.g., cellular), or this device can accept and/or transmit data messages or video content via an unregulated spectrum (e.g., WiFi) connection.

Mobile device 1000 includes scanning laser projector 1020, touch sensitive display 1010, audio port 1002, control buttons 1004, card slot 1006, and audio/video (A/V) port 1008. None of these elements are essential. For example, mobile device may only include scanning laser projector 1020 without any of touch sensitive display 1010, audio port 1002, control buttons 1004, card slot 1006, or A/V port 1008. Some embodiments include a subset of these elements. For example, an accessory projector may include scanning laser projector 1020, control buttons 1004 and A/V port 1008. A smartphone embodiment may combine touch sensitive display device 1010 and projector 1020.

Touch sensitive display 1010 may be any type of display. For example, in some embodiments, touch sensitive display 1010 includes a liquid crystal display (LCD) screen. In some embodiments, display 1010 is not touch sensitive. Display 1010 may or may not always display the image projected by scanning laser projector 1020. For example, an accessory product may always display the projected image on display 1010, whereas a mobile phone embodiment may project a video while displaying different content on display 1010. Some embodiments may include a keypad in addition to touch sensitive display 1010. A/V port 1008 accepts and/or transmits video and/or audio signals. For example, A/V port 1008 may be a digital port, such as a high definition multimedia interface (HDMI) interface that accepts a cable suitable to carry digital audio and video data. Further, A/V port 1008 may include RCA jacks to accept or transmit composite inputs. Still further, A/V port 1008 may include a VGA connector to accept or transmit analog video signals.

In some embodiments, mobile device 1000 may be tethered to an external signal source through A/V port 1008, and mobile device 1000 may project content accepted through A/V port 1008. In other embodiments, mobile device 1000 may be an originator of content, and A/V port 1008 is used to transmit content to a different device.

Audio port 1002 provides audio signals. For example, in some embodiments, mobile device 1000 is a media recorder that can record and play audio and video. In these embodiments, the video may be projected by scanning laser projector 1020 and the audio may be output at audio port 1002.

Mobile device 1000 also includes card slot 1006. In some embodiments, a memory card inserted in card slot 1006 may provide a source for audio to be output at audio port 1002 and/or video data to be projected by scanning laser projector 1020. Card slot 1006 may receive any type of solid state memory device, including for example secure digital (SD) memory cards.

Turning to FIG. 9, a perspective view of a head-up display system 1100 in accordance with various embodiments is illustrated. Specifically, head-up display system 1100 is an example of the type of device in which a scanning laser projector as described above can be implemented (e.g., scanning laser projector 100, scanning laser projector 700). The head-up display system 1100 includes a scanning laser projector 1102. Specifically, the scanning laser projector 1102 is shown mounted in a vehicle dash to project the head-up display. Although an automotive head-up display is shown in FIG. 9, this is not a limitation and other applications are possible. For example, various embodiments include head-up displays in avionics application, air traffic control applications, and other applications.

Turning to FIG. 10, a perspective view of eyewear 1200 in accordance with various embodiments is illustrated. Specifically, eyewear 1200 is an example of the type of device in which a scanning laser projector as described above can be implemented (e.g., scanning laser projector 100, scanning laser projector 700). Eyewear 1200 includes scanning laser projector 1202 to project a display in the eyewear's field of view. In some embodiments, eyewear 1200 is see-through and in other embodiments, eyewear 1200 is opaque. For example, eyewear 1200 may be used in an augmented reality application in which a wearer can see the display from projector 1202 overlaid on the physical world. Also for example, eyewear 1200 may be used in a virtual reality application, in which a wearer's entire view is generated by projector 1202.

Although only one projector 1202 is shown in FIG. 10, this is not a limitation and other implementations are possible. For example, in some embodiments, eyewear 1200 includes two projectors 1202, with one for each eye

Turning to FIG. 11, a perspective view of a gaming apparatus 1300 in accordance with various embodiments is illustrated. Gaming apparatus 1300 allows a user or users to observe and interact with a gaming environment. In some embodiments, the game is navigated based on the motion, position, or orientation of gaming apparatus 1300, an apparatus that includes scanning laser projector 1302. Other control interfaces, such as manually-operated buttons, foot pedals, or verbal commands, may also contribute to navigation around, or interaction with the gaming environment. For example, in some embodiments, trigger 1342 contributes to the illusion that the user or users are in a first person perspective video game environment, commonly known as a “first person shooter game.” Because the size and brightness of the projected display can be controlled by the gaming application in combination with the user's movement, gaming apparatus 1300 creates a highly believable or “immersive” environment for these users.

Many other first person perspective simulations can also be created by gaming apparatus 1300, for such activities as 3D seismic geo-prospecting, spacewalk planning, jungle canopy exploration, automobile safety instruction, medical education, etc. Tactile interface 1344 may provide a variety of output signals, such as recoil, vibration, shake, rumble, etc. Tactile interface 1344 may also include a touch-sensitive input feature, such as a touch sensitive display screen or a display screen that requires a stylus. Additional tactile interfaces, for example, input and/or output features for a motion sensitive probe are also included in various embodiments of the present invention.

Gaming apparatus 1300 may also include audio output devices, such as integrated audio speakers, remote speakers, or headphones. These sorts of audio output devices may be connected to gaming apparatus 1300 with wires or through a wireless technology. For example, wireless headphones 1346 provide the user with sound effects via a BLUETOOTH™ connection, although any sort of similar wireless technology could be substituted freely. In some embodiments, wireless headphones 1346 may include microphone 1345 or binaural microphone 1347, to allow multiple users, instructors, or observers to communicate. Binaural microphone 1347 typically includes microphones on each ear piece, to capture sounds modified by the user's head shadow. This feature may be used for binaural hearing and sound localization by other simulation participants.

Gaming apparatus 1300 may include any number of sensors 1310 that measure ambient brightness, motion, position, orientation, and the like. For example, gaming apparatus 1300 may detect absolute heading with a digital compass, and detect relative motion with an x-y-z gyroscope or accelerometer. In some embodiments, gaming apparatus 1300 also includes a second accelerometer or gyroscope to detect the relative orientation of the device, or its rapid acceleration or deceleration. In other embodiments, gaming apparatus 1300 may include a Global Positioning Satellite (GPS) sensor, to detect absolute position as the user travels in terrestrial space.

Gaming apparatus 1300 may include battery 1341 and/or diagnostic lights 1343. For example, battery 1341 may be a rechargeable battery, and diagnostic lights 1343 could indicate the current charge of the battery. In another example, battery 1341 may be a removable battery clip, and gaming apparatus 1300 may have an additional battery, electrical capacitor or super-capacitor to allow for continued operation of the apparatus while the discharged battery is replaced with a charged battery. In other embodiments, diagnostic lights 1343 can inform the user or a service technician about the status of the electronic components included within or connected to this device. For example, diagnostic lights 1343 may indicate the strength of a received wireless signal, or the presence or absence of a memory card.

Diagnostic lights 1343 could also be replaced by any small screen, such as an organic light emitting diode or liquid crystal display screen. Such lights or screens could be on the exterior surface of gaming apparatus 1300, or below the surface, if the shell for this apparatus is translucent or transparent. Other components of gaming apparatus 1300 may be removable, detachable or separable from this device. For example, scanning laser projector 1302 may be detachable or separable from gaming housing 1389. In some embodiments, the subcomponents of scanning laser projector 100 may be detachable or separable from gaming housing 1389, and still function.

Turning to FIG. 12, a perspective view of a gaming apparatus 1400 in accordance with various embodiments is illustrated. Gaming apparatus 1400 includes buttons 1404, display 1410, and projector 1402. In some embodiments, gaming apparatus 1400 is a standalone apparatus that does not need a larger console for a user to play a game. For example, a user may play a game while watching display 1410 and/or the projected content. In other embodiments, gaming apparatus 1400 operates as a controller for a larger gaming console. In these embodiments, a user may watch a larger screen tethered to the console in combination with watching display 1410 and/or projected content.

In a first embodiment, a scanning laser projector is provided, comprising: at least one source of laser light; a first solid figure element, a polarizing beam splitter, and an array of mirrors, the array of mirrors including at least two reflecting surfaces, the polarizing beam splitter positioned between the first solid figure element and the array of mirrors, the first solid figure element configured to receive the laser light and pass the laser light to the polarizing beam splitter, the polarizing beam splitter configured to pass a first portion of the laser light having a first polarization to the array of mirrors, and reflect a second portion of the laser light having a second polarization back to the first solid figure element, the array of mirrors configured to reflect the first portion of the laser light off the at least two reflecting surfaces and direct the reflected first portion of the laser light back into the first solid figure element, and wherein the reflected first portion of the laser light is spatially recombined with the second portion of the laser light in the first solid figure element to form a recombined laser light beam, and wherein the first solid figure element outputs the recombined laser light; at least one scanning mirror configured to reflect the recombined laser light beam; and a drive circuit configured to provide an excitation signal to excite motion of the scanning mirror to reflect the recombined laser light beam in a pattern of scan lines.

In another embodiment, a scanning laser projector is provided, comprising: at least one source of laser light, the laser light having substantially linear polarization; a speckle reduction component, the speckle reduction component configured to receive the laser light, the speckle reduction component including: a polarization adjuster, the polarization adjuster configured to receive the laser light and convert the laser light to orthogonally polarized light having orthogonal polarization components with equal optical power; and a prism element, a polarizing beam splitter, a polyhedron element, a first mirror and a second mirror, the polarizing beam splitter positioned between the prism element and the polyhedron element, the prism element configured to receive the laser light from the polarization adjuster and pass the laser light to the polarizing beam splitter, the polarizing beam splitter configured to pass a first portion of the laser light having a P polarization to the polyhedron element, and reflect a second portion of the having a S polarization back to the prism element, the polyhedron element having at least four surfaces, and with a first of the four surfaces adjacent to the prism element, and wherein the first mirror is affixed to a second of the four surfaces with index matching adhesive, and wherein the second mirror is affixed to a third of the four surfaces with index matching adhesive, and wherein the first mirror and the second mirror are configured to provide reflection of the first portion of the laser light and then output the first portion of the laser light into the prism element, and wherein the first mirror is positioned relative to the second of the four surfaces and the second mirror is positioned relative to the third of the four surfaces to spatially recombine the first portion of the laser light with the second portion in the prism element to generate a recombined laser light beam, and wherein the prism element outputs the recombined laser light beam; at least one scanning mirror configured to reflect the recombined laser light beam; and a drive circuit configured to provide an excitation signal to excite motion of the scanning mirror to reflect the recombined laser light beam in a pattern of scan lines.

In the preceding detailed description, reference was made to the accompanying drawings that show, by way of illustration, specific embodiments in which the invention may be practiced. These embodiments were described in sufficient detail to enable those skilled in the art to practice the invention. It is to be understood that the various embodiments of the invention, although different, are not necessarily mutually exclusive. For example, a particular feature, structure, or characteristic described herein in connection with one embodiment may be implemented within other embodiments without departing from the scope of the invention. In addition, it is to be understood that the location or arrangement of individual elements within each disclosed embodiment may be modified without departing from the scope of the invention. The preceding detailed description is, therefore, not to be taken in a limiting sense, and the scope of the present invention is defined only by the appended claims, appropriately interpreted, along with the full range of equivalents to which the claims are entitled. In the drawings, like numerals refer to the same or similar functionality throughout the several views.

Although the present invention has been described in conjunction with certain embodiments, it is to be understood that modifications and variations may be resorted to without departing from the scope of the invention as those skilled in the art readily understand. Such modifications and variations are considered to be within the scope of the invention and the appended claims. 

What is claimed is:
 1. A scanning laser projector, comprising: at least one source of laser light; a first solid figure element, a polarizing beam splitter, and an array of mirrors, the array of mirrors including at least two reflecting surfaces, the polarizing beam splitter positioned between the first solid figure element and the array of mirrors, the first solid figure element configured to receive the laser light and pass the laser light to the polarizing beam splitter, the polarizing beam splitter configured to pass a first portion of the laser light having a first polarization to the array of mirrors, and reflect a second portion of the laser light having a second polarization back to the first solid figure element, the array of mirrors configured to reflect the first portion of the laser light off the at least two reflecting surfaces and direct the reflected first portion of the laser light back into the first solid figure element, and wherein the reflected first portion of the laser light is spatially recombined with the second portion of the laser light in the first solid figure element to form a recombined laser light beam, and wherein the first solid figure element outputs the recombined laser light; at least one scanning mirror configured to reflect the recombined laser light beam; and a drive circuit configured to provide an excitation signal to excite motion of the scanning mirror to reflect the recombined laser light beam in a pattern of scan lines.
 2. The scanning laser projector of claim 1, wherein the array of mirrors includes at least a first mirror and a second mirror, and wherein the first mirror and the second mirror are positioned to make the first portion of the laser light coaxial with the second portion of the laser light when spatially recombined in the first solid figure element.
 3. The scanning laser projector of claim 2, wherein the first mirror and the second mirror have configured to have adjustable positions to facilitate precise positioning of the first mirror and the second mirror.
 4. The scanning laser projector of claim 2, wherein the array of mirrors includes at least a third mirror.
 5. The scanning laser projector of claim 1, wherein the first solid figure element comprises a prism.
 6. The scanning laser projector of claim 1, further comprising a second solid figure element having at least a first surface, a second surface, and a third surface, and wherein the array of mirrors includes at least a first mirror and a second mirror, the first wherein the first mirror is attached to the first surface and the second mirror is attached to the second surface.
 7. The scanning laser projector of claim 6, wherein the third surface is configured to provide total internal reflection of the first portion of the laser light.
 8. The scanning laser projector of claim 6, wherein the array of mirrors includes a third mirror, and wherein the third mirror is attached to the third surface to provide reflection of the first portion of the laser light.
 9. The scanning laser projector of claim 6, wherein at least the first mirror and the second mirror are positioned to make the first portion of the laser light coaxial with the second portion of the laser light when spatially recombined in the first solid figure element.
 10. The scanning laser projector of claim 6, wherein the first mirror is attached to the first surface with index matching adhesive and the second mirror is attached to the second surface with index matching adhesive.
 11. The scanning laser projector of claim 6, wherein the first mirror is attached to the first surface with index matching adhesive and the second mirror is attached to the second surface with index matching adhesive, and wherein at the first mirror and the second mirror are positioned with the index matching adhesive to make the first portion of the laser light coaxial with the second portion of the laser light when spatially recombined in the first solid figure element.
 12. The scanning laser projector of claim 6, wherein the second solid figure element comprises a polyhedron.
 13. The scanning laser projector of claim 1, wherein the first polarization comprises a P polarization and wherein the second polarization comprises an S polarization.
 14. The scanning laser projector of claim 1, further comprising a polarization adjuster, the polarization adjuster configured to receive the laser light from the at least one source of laser light and further configured to adjust the laser light to have optical power along two orthogonal polarizations.
 15. The scanning laser projector of claim 1, wherein the array of mirrors is configured to introduce a relative delay between the first portion of the laser light and the second portion of the laser light, where the relative delay is greater than a coherence length of the laser light.
 16. The scanning laser projector of claim 15, wherein the coherence length is defined as $L_{c} = \frac{\lambda^{2}}{\Delta\;\lambda}$ where λ is the central wavelength of the laser light, and Δλ is a full width half maximum (FWHM) spectral bandwidth of the laser light.
 17. The scanning laser projector of claim 1, wherein the polarizing beam splitter comprises a coating applied to the first solid figure element.
 18. The scanning laser projector of claim 1, wherein the laser light has a non-circular spatial distribution when received at the first solid figure element, and wherein the first solid figure element has an input surface and an output surface, and wherein the output surface is configured such that the recombined laser light beam is output at a non-orthogonal angle to the output surface and is spatially circularized upon exiting the output surface.
 19. The scanning laser projector of claim 1, wherein the first solid figure element has an input surface and an output surface, and wherein an anti-reflective coating is applied to both the input surface and the output surface.
 20. A scanning laser projector, comprising: at least one source of laser light, the laser light having substantially linear polarization; a speckle reduction component, the speckle reduction component configured to receive the laser light, the speckle reduction component including: a polarization adjuster, the polarization adjuster configured to receive the laser light and convert the laser light to orthogonally polarized light having orthogonal polarization components with equal optical power; and a prism element, a polarizing beam splitter, a polyhedron element, a first mirror and a second mirror, the polarizing beam splitter positioned between the prism element and the polyhedron element, the prism element configured to receive the laser light from the polarization adjuster and pass the laser light to the polarizing beam splitter, the polarizing beam splitter configured to pass a first portion of the laser light having a P polarization to the polyhedron element, and reflect a second portion of the having a S polarization back to the prism element, the polyhedron element having at least four surfaces, and with a first of the four surfaces adjacent to the prism element, and wherein the first mirror is affixed to a second of the four surfaces with index matching adhesive, and wherein the second mirror is affixed to a third of the four surfaces with index matching adhesive, and wherein the first mirror and the second mirror are configured to provide reflection of the first portion of the laser light and then output the first portion of the laser light into the prism element, and wherein the first mirror is positioned relative to the second of the four surfaces and the second mirror is positioned relative to the third of the four surfaces to spatially recombine the first portion of the laser light with the second portion in the prism element to generate a recombined laser light beam, and wherein the prism element outputs the recombined laser light beam; at least one scanning mirror configured to reflect the recombined laser light beam; and a drive circuit configured to provide an excitation signal to excite motion of the scanning mirror to reflect the recombined laser light beam in a pattern of scan lines. 